相关实验视频
Updated: Jun 12, 2025

10:59
Analysis of SEC-SAXS data via EFA deconvolution and Scatter
Published on: January 28, 2021
9.0K
和原子对原子对相关性之间的麦克斯韦尔关系
Raymon S Watson1, Caleb Coleman1, Karen V Kheruntsyan1
1School of Mathematics and Physics, <a href="https://ror.org/00rqy9422">University of Queensland</a>, Brisbane, Queensland 4072, Australia.
Physical review letters
|September 20, 2024
概括
研究人员得出了麦克斯韦关系,将粒子对相关性与1D波斯气体的相连接. 这允许从易于测量的相关性计算,简化量子气体分析.
科学领域:
- 量子物理学的量子物理学
- 热力学是一种热力学.
- 统计力学就是统计力学.
背景情况:
- 局部粒子对相关函数是多粒子系统中的热力学量.
- 赫尔曼-费曼定理允许计算这些相关性.
- 量子气体中的值计算在计算上具有挑战性.
研究的目的:
- 导出局部对相关性和之间的热力学麦克斯韦关系.
- 应用这个关系来确定1D波斯气体的.
- 展示一种用于测量量子气体的新方法.
主要方法:
- 利用赫尔曼-费曼定理来确定局部对相关性的热力学属性.
- 导出了麦克斯韦关系,将局部对相关性与联系起来.
- 在随机预测的Gross-Pitaevskii方程 (SPGPE) 形式主义中应用了衍生关系.
主要成果:
- 成功推导出1D波斯气体的麦克斯韦关系.
- 证明了从原子-原子对相关函数可以确定.
- 展示了通过相关函数计算计算的可行性.
结论:
- 派生的麦克斯韦关系提供了可测量的相关性和之间的实际联系.
- 这种方法简化了有限温度1D斯气体的度确定.
- 提出了一种实验技术的原理证明,用于从相关性中测量量子气体.
相关概念视频
Entropy
28.9K
Salt particles that have dissolved in water never spontaneously come back together in solution to reform solid particles. Moreover, a gas that has expanded in a vacuum remains dispersed and never spontaneously reassembles. The unidirectional nature of these phenomena is the result of a thermodynamic state function called entropy (S). Entropy is the measure of the extent to which the energy is dispersed throughout a system, or in other words, it is proportional to the degree of disorder of a...
28.9K
Maxwell's Thermodynamic Relations
2.6K
Maxwell's thermodynamic relations are very useful in solving problems in thermodynamics. Each of Maxwell's relations relates a partial differential between quantities that can be hard to measure experimentally to a partial differential between quantities that can be easily measured. These relations are a set of equations derivable from the symmetry of the second derivatives and the thermodynamic potentials.
All thermodynamic potentials are exact differentials. Therefore, their second-order...
All thermodynamic potentials are exact differentials. Therefore, their second-order...
2.6K
Third Law of Thermodynamics
18.3K
A pure, perfectly crystalline solid possessing no kinetic energy (that is, at a temperature of absolute zero, 0 K) may be described by a single microstate, as its purity, perfect crystallinity,and complete lack of motion means there is but one possible location for each identical atom or molecule comprising the crystal (W = 1). According to the Boltzmann equation, the entropy of this system is zero.
18.3K
Entropy and the Second Law of Thermodynamics
2.8K
The second law of thermodynamics can be stated quantitatively using the concept of entropy. Entropy is the measure of disorder of the system.
The relation between entropy and disorder can be illustrated with the example of the phase change of ice to water. In ice, the molecules are located at specific sites giving a solid state, whereas, in a liquid form, these molecules are much freer to move. The molecular arrangement has therefore become more randomized. Although the change in average...
The relation between entropy and disorder can be illustrated with the example of the phase change of ice to water. In ice, the molecules are located at specific sites giving a solid state, whereas, in a liquid form, these molecules are much freer to move. The molecular arrangement has therefore become more randomized. Although the change in average...
2.8K
The Second Law of Thermodynamics
5.2K
In the quest to identify a property that may reliably predict the spontaneity of a process, a promising candidate has been identified: entropy. Scientists refer to the measure of randomness or disorder within a system as entropy. High entropy means high disorder and low energy. To better understand entropy, think of a student’s bedroom. If no energy or work were put into it, the room would quickly become messy. It would exist in a very disordered state, one of high entropy. Energy must be...
5.2K
The Quantum-Mechanical Model of an Atom
42.1K
Shortly after de Broglie published his ideas that the electron in a hydrogen atom could be better thought of as being a circular standing wave instead of a particle moving in quantized circular orbits, Erwin Schrödinger extended de Broglie’s work by deriving what is now known as the Schrödinger equation. When Schrödinger applied his equation to hydrogen-like atoms, he was able to reproduce Bohr’s expression for the energy and, thus, the Rydberg formula governing hydrogen spectra.
42.1K

